Note
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PF: Gravity: Tiled Inversion Linear¶
Invert data in tiles.
import numpy as np
import matplotlib.pyplot as plt
from discretize import TensorMesh
from SimPEG.potential_fields import gravity
from SimPEG import (
maps,
data,
data_misfit,
regularization,
optimization,
inverse_problem,
directives,
inversion,
)
from discretize.utils import mesh_builder_xyz, refine_tree_xyz
try:
from SimPEG import utils
from SimPEG.utils import plot2Ddata
except:
from SimPEG import Utils as utils
from SimPEG.Utils.Plotutils import plot2Ddata
import shutil
Setup¶
Define the survey and model parameters
Create an a global survey and mesh and simulate some data
# Create and array of observation points
xr = np.linspace(-30.0, 30.0, 20)
yr = np.linspace(-30.0, 30.0, 20)
X, Y = np.meshgrid(xr, yr)
# Move the observation points 5m above the topo
Z = -np.exp((X ** 2 + Y ** 2) / 75 ** 2)
# Create a topo array
topo = np.c_[utils.mkvc(X.T), utils.mkvc(Y.T), utils.mkvc(Z.T)]
# Create station locations drapped 0.1 m above topo
rxLoc = np.c_[utils.mkvc(X.T), utils.mkvc(Y.T), utils.mkvc(Z.T) + 0.1]
Divided and Conquer¶
Split the data set in two and create sub-problems
# Mesh parameters
h = [5, 5, 5]
padDist = np.ones((3, 2)) * 100
octree_levels = [8, 4]
# Create tiles
local_indices = [rxLoc[:, 0] <= 0, rxLoc[:, 0] > 0]
local_surveys = []
local_meshes = []
for local_index in local_indices:
receivers = gravity.receivers.Point(rxLoc[local_index, :])
srcField = gravity.sources.SourceField([receivers])
local_survey = gravity.survey.Survey(srcField)
# Create a local mesh that covers all points, but refined on the local survey
local_mesh = mesh_builder_xyz(
topo, h, padding_distance=padDist, depth_core=100, mesh_type="tree"
)
local_mesh = refine_tree_xyz(
local_mesh,
local_survey.receiver_locations,
method="surface",
octree_levels=octree_levels,
finalize=True,
)
local_surveys.append(local_survey)
local_meshes.append(local_mesh)
Global Mesh¶
Create a global mesh survey for simulation
mesh = mesh_builder_xyz(
topo, h, padding_distance=padDist, depth_core=100, mesh_type="tree"
)
# This garantees that the local meshes are always coarser or equal
for local_mesh in local_meshes:
mesh.insert_cells(
local_mesh.gridCC,
local_mesh.cell_levels_by_index(np.arange(local_mesh.nC)),
finalize=False,
)
mesh.finalize()
# Define an active cells from topo
activeCells = utils.surface2ind_topo(mesh, topo)
nC = int(activeCells.sum())
# We can now create a density model and generate data
# Here a simple block in half-space
# Get the indicies of the magnetized block
model = np.zeros(mesh.nC)
ind = utils.ModelBuilder.getIndicesBlock(
np.r_[-10, -10, -30], np.r_[10, 10, -10], mesh.gridCC,
)[0]
# Assign magnetization values
model[ind] = 0.3
# Remove air cells
model = model[activeCells]
# Create reduced identity map
idenMap = maps.IdentityMap(nP=nC)
# Create a global survey just for simulation of data
receivers = gravity.receivers.Point(rxLoc)
srcField = gravity.sources.SourceField([receivers])
survey = gravity.survey.Survey(srcField)
# Create the forward simulation for the global dataset
simulation = gravity.simulation.Simulation3DIntegral(
survey=survey, mesh=mesh, rhoMap=idenMap, actInd=activeCells
)
# Compute linear forward operator and compute some data
d = simulation.fields(model)
# Add noise and uncertainties
# We add some random Gaussian noise (1nT)
synthetic_data = d + np.random.randn(len(d)) * 1e-3
wd = np.ones(len(synthetic_data)) * 1e-3 # Assign flat uncertainties
Tiled misfits
local_misfits = []
for ii, local_survey in enumerate(local_surveys):
tile_map = maps.TileMap(mesh, activeCells, local_meshes[ii])
local_actives = tile_map.local_active
# Create the forward simulation
simulation = gravity.simulation.Simulation3DIntegral(
survey=local_survey,
mesh=local_meshes[ii],
rhoMap=tile_map,
actInd=local_actives,
sensitivity_path=f"Inversion\Tile{ii}.zarr",
)
data_object = data.Data(
local_survey,
dobs=synthetic_data[local_indices[ii]],
standard_deviation=wd[local_indices[ii]],
)
local_misfits.append(
data_misfit.L2DataMisfit(data=data_object, simulation=simulation)
)
# Our global misfit
global_misfit = local_misfits[0] + local_misfits[1]
# Plot the model on different meshes
fig = plt.figure(figsize=(12, 6))
for ii, local_misfit in enumerate(local_misfits):
local_mesh = local_misfit.simulation.mesh
local_map = local_misfit.simulation.rhoMap
inject_local = maps.InjectActiveCells(local_mesh, local_map.local_active, np.nan)
ax = plt.subplot(2, 2, ii + 1)
local_mesh.plotSlice(
inject_local * (local_map * model), normal="Y", ax=ax, grid=True
)
ax.set_aspect("equal")
ax.set_title(f"Mesh {ii+1}. Active cells {local_map.local_active.sum()}")
# Create active map to go from reduce set to full
inject_global = maps.InjectActiveCells(mesh, activeCells, np.nan)
ax = plt.subplot(2, 1, 2)
mesh.plotSlice(inject_global * model, normal="Y", ax=ax, grid=True)
ax.set_title(f"Global Mesh. Active cells {activeCells.sum()}")
ax.set_aspect("equal")
plt.show()
Out:
/Users/josephcapriotti/codes/simpeg/examples/02-gravity/plot_inv_grav_tiled.py:217: UserWarning: Matplotlib is currently using agg, which is a non-GUI backend, so cannot show the figure.
plt.show()
Invert on the global mesh
# Create reduced identity map
idenMap = maps.IdentityMap(nP=nC)
# Create a regularization
reg = regularization.Sparse(mesh, indActive=activeCells, mapping=idenMap)
m0 = np.ones(nC) * 1e-4 # Starting model
# Add directives to the inversion
opt = optimization.ProjectedGNCG(
maxIter=100, lower=-1.0, upper=1.0, maxIterLS=20, maxIterCG=10, tolCG=1e-3
)
invProb = inverse_problem.BaseInvProblem(global_misfit, reg, opt)
betaest = directives.BetaEstimate_ByEig(beta0_ratio=1e-1)
# Here is where the norms are applied
# Use pick a threshold parameter empirically based on the distribution of
# model parameters
update_IRLS = directives.Update_IRLS(
f_min_change=1e-4, max_irls_iterations=0, coolEpsFact=1.5, beta_tol=1e-2,
)
saveDict = directives.SaveOutputEveryIteration(save_txt=False)
update_Jacobi = directives.UpdatePreconditioner()
sensitivity_weights = directives.UpdateSensitivityWeights(everyIter=False)
inv = inversion.BaseInversion(
invProb,
directiveList=[update_IRLS, sensitivity_weights, betaest, update_Jacobi, saveDict],
)
# Run the inversion
mrec = inv.run(m0)
# Plot the result
ax = plt.subplot(1, 2, 1)
mesh.plotSlice(inject_global * model, normal="Y", ax=ax, grid=True)
ax.set_title("True")
ax.set_aspect("equal")
ax = plt.subplot(1, 2, 2)
mesh.plotSlice(inject_global * mrec, normal="Y", ax=ax, grid=True)
ax.set_title("Recovered")
ax.set_aspect("equal")
plt.show()
Out:
SimPEG.InvProblem will set Regularization.mref to m0.
SimPEG.InvProblem is setting bfgsH0 to the inverse of the eval2Deriv.
***Done using same Solver and solver_opts as the Simulation3DIntegral problem***
model has any nan: 0
=============================== Projected GNCG ===============================
# beta phi_d phi_m f |proj(x-g)-x| LS Comment
-----------------------------------------------------------------------------
x0 has any nan: 0
0 3.49e+06 4.21e+04 0.00e+00 4.21e+04 4.80e+01 0
1 1.75e+06 4.42e+03 1.07e-03 6.29e+03 4.77e+01 0
2 8.73e+05 2.36e+03 1.91e-03 4.02e+03 4.74e+01 0 Skip BFGS
3 4.37e+05 1.12e+03 2.89e-03 2.38e+03 4.72e+01 0 Skip BFGS
4 2.18e+05 5.34e+02 3.82e-03 1.37e+03 4.67e+01 0 Skip BFGS
5 1.09e+05 2.90e+02 4.58e-03 7.90e+02 4.61e+01 0 Skip BFGS
Reached starting chifact with l2-norm regularization: Start IRLS steps...
eps_p: 0.07141989320928005 eps_q: 0.07141989320928005
Reach maximum number of IRLS cycles: 0
------------------------- STOP! -------------------------
1 : |fc-fOld| = 0.0000e+00 <= tolF*(1+|f0|) = 4.2128e+03
1 : |xc-x_last| = 3.8487e-02 <= tolX*(1+|x0|) = 1.0048e-01
0 : |proj(x-g)-x| = 4.6036e+01 <= tolG = 1.0000e-01
0 : |proj(x-g)-x| = 4.6036e+01 <= 1e3*eps = 1.0000e-02
0 : maxIter = 100 <= iter = 6
------------------------- DONE! -------------------------
/Users/josephcapriotti/codes/simpeg/examples/02-gravity/plot_inv_grav_tiled.py:271: UserWarning: Matplotlib is currently using agg, which is a non-GUI backend, so cannot show the figure.
plt.show()
Total running time of the script: ( 0 minutes 4.024 seconds)